<resource xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns="http://datacite.org/schema/kernel-4" xsi:schemaLocation="http://datacite.org/schema/kernel-4 http://schema.datacite.org/meta/kernel-4.1/metadata.xsd"><identifier identifierType="DOI">10.26165/JUELICH-DATA/EDREBI</identifier><creators><creator><creatorName>Zsurka, Eduárd</creatorName><affiliation>PGI-9 / JARA-FIT / Department of Physics and Materials Science, University of Luxembourg, 1511 Luxembourg, Luxembourg</affiliation></creator><creator><creatorName nameType="Personal">Wang, Cheng</creatorName><givenName>Cheng</givenName><familyName>Wang</familyName><affiliation>PGI-1</affiliation></creator><creator><creatorName nameType="Personal">Legendre, Julian</creatorName><givenName>Julian</givenName><familyName>Legendre</familyName><affiliation>Department of Physics and Materials Science, University of Luxembourg, 1511 Luxembourg, Luxembourg</affiliation></creator><creator><creatorName nameType="Personal">Di Miceli, Daniele</creatorName><givenName>Daniele</givenName><familyName>Di Miceli</familyName><affiliation>Department of Physics and Materials Science, University of Luxembourg, 1511 Luxembourg, Luxembourg</affiliation></creator><creator><creatorName>Serra, Llorenç</creatorName><affiliation>Institute for Cross-Disciplinary Physics and Complex Systems IFISC (CSIC-UIB), E-07122 Palma, Spain / Department of Physics, University of the Balearic Islands, E-07122 Palma, Spain</affiliation></creator><creator><creatorName nameType="Personal">Grützmacher, Detlev</creatorName><givenName>Detlev</givenName><familyName>Grützmacher</familyName><affiliation>PGI-9 / JARA-FIT</affiliation></creator><creator><creatorName nameType="Personal">Schmidt, Thomas L.</creatorName><givenName>Thomas L.</givenName><familyName>Schmidt</familyName><affiliation>Department of Physics and Materials Science, University of Luxembourg, 1511 Luxembourg, Luxembourg</affiliation></creator><creator><creatorName nameType="Personal">Rüßmann, Philipp</creatorName><givenName>Philipp</givenName><familyName>Rüßmann</familyName><affiliation>PGI-1 /  Institute for Theoretical Physics and Astrophysics, University of Würzburg, 97074 Würzburg, Germany</affiliation></creator><creator><creatorName nameType="Personal">Moors, Kristof</creatorName><givenName>Kristof</givenName><familyName>Moors</familyName><affiliation>PGI-9 / JARA-FIT</affiliation></creator></creators><titles><title>Replication Data for: Low-energy modeling of three-dimensional topological insulator nanostructures</title></titles><publisher>Jülich DATA</publisher><publicationYear>2024</publicationYear><subjects><subject>Physics</subject><subject>DFT</subject><subject>topological insulators</subject><subject>tight-binding</subject><subject>k.p low energy model</subject><subject>effective Hamiltonian</subject></subjects><contributors><contributor contributorType="ContactPerson"><contributorName nameType="Personal">Rüßmann, Philipp</contributorName><givenName>Philipp</givenName><familyName>Rüßmann</familyName><affiliation>PGI-1</affiliation></contributor></contributors><dates><date dateType="Submitted">2024-07-05</date><date dateType="Updated">2024-07-05</date></dates><resourceType resourceTypeGeneral="Dataset"/><relatedIdentifiers><relatedIdentifier relationType="IsCitedBy" relatedIdentifierType="DOI">10.24435/materialscloud:mx-bn</relatedIdentifier></relatedIdentifiers><version>1.0</version><rightsList><rights rightsURI="info:eu-repo/semantics/openAccess"/><rights rightsURI="https://creativecommons.org/publicdomain/zero/1.0/">CC0 Waiver</rights></rightsList><descriptions><description descriptionType="Abstract">We develop an accurate nanoelectronic modeling approach for realistic three-dimensional topological insulator nanostructures and investigate their low-energy surface-state spectrum. Starting from the commonly considered four-band k·p bulk model Hamiltonian for the Bi₂Se₃ family of topological insulators, we derive new parameter sets for Bi₂Se₃, Bi₂Te₃ and Sb₂Te₃. We consider a fitting strategy applied to ab initio band structures around the Γ point that ensures a quantitatively accurate description of the low-energy bulk and surface states, while avoiding the appearance of unphysical low-energy states at higher momenta, something that is not guaranteed by the commonly considered perturbative approach. We analyze  the effects that arise in the low-energy spectrum of topological surface states due to band anisotropy and electron-hole asymmetry, yielding Dirac surface states that naturally localize on different side facets. In the thin-film limit, when surface states hybridize through the bulk, we resort to a thin-film model and derive thickness-dependent model parameters from ab initio calculations that show good agreement with experimentally resolved band structures, unlike the bulk model that neglects relevant many-body effects in this regime. Our versatile modeling approach offers a reliable starting point for accurate simulations of realistic topological material-based nanoelectronic devices.&#xd;
This dataset contains the data used in the corresponding publication.</description></descriptions><geoLocations/></resource>